Flux density inside and outside a coaxial cable.

AI Thread Summary
The discussion focuses on calculating the magnetic field (B) inside and outside a coaxial cable. For the region outside the coaxial cable, the magnetic field is derived as B = (μI)/(2∏r), while the calculation for inside the coaxial cable appears to be misinterpreted, as it suggests a scenario not asked in the problem. The inner current flows leftward and the outer current flows rightward, leading to confusion about the total current piercing the area outside the outer mesh. Additionally, the region between the conductors is filled with an insulator, which does not allow current flow. The calculations need clarification to align with the problem's requirements.
lam58
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For question 4b in the problem sheet attached below, is my working correct for B outside and inside the coaxial cable?




Ans:

Outside coaxial:∫B.dl = μI (the integral is between 0 and 2∏r)
=> B = (μI)/(2∏r)

Inside the coaxial: \int_{2\pi a}^{2\pi r} B.dI
= μI.\frac{a^2}{\pi r^{2}b^{2}}

=> B[2\pi r - 2\pi a] = μI.\frac{a^2}{\pi r^{2}b^{2}}
=>B = μI.\frac{a^2}{\pi r^{2}b^{2}} * \frac{1}{2\pi r - 2\pi a}
 

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It's not obvious what you mean by "outside the coaxial" ... do you mean "between the conductors"?
Notice that the inner current Ia is leftward, but the outer current Ib is rightward.
So, for r>b (outside the outer mesh), how much total I is piercing the Area?

It looks like your "inside the coaxial" is trying to be for r<a, that is, inside the inner conducting wire, assuming uniform current density. This region was not asked for in the problem (perhaps because the current density is not really uniform, in real situations). The region between a and b is filled with insulator, having zero current flow in it (so the right-hand side is constant non-zero).
 
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